ENTRY C2215 20160512 C160C2215 0 1 SUBENT C2215001 20160512 C160C2215 1 1 BIB 11 44 C2215 1 2 TITLE Angle-integrated measurements of the 26Al(d,n)27Si C2215 1 3 reaction cross section: a probe of spectroscopic C2215 1 4 factors and astrophysical resonance strengths C2215 1 5 AUTHOR (A.Kankainen,P.J.Woods,F.Nunes,C.Langer,H.Schatz, C2215 1 6 V.Bader,T.Baugher,D.Bazin,B.A.Brown,J.Browne, C2215 1 7 D.T.Doherty,A.Estrade,A.Gade,A.Kontos,G.Lotay,Z.Meisel,C2215 1 8 F.Montes,S.Noji,G.Perdikakis,J.Pereira,F.Recchia, C2215 1 9 T.Redpath,R.Stroberg,M.Scott,D.Seweryniak,J.Stevens, C2215 1 10 D.Weisshaar,K.Wimmer,R.Zegers) C2215 1 11 INSTITUTE (2UK EDG,1USAMSU,1USAANL) C2215 1 12 (1USAUSA) Central Michigan University, Mount Pleasant, C2215 1 13 Michigan C2215 1 14 REFERENCE (J,EPJ/A,52,6,2016) C2215 1 15 FACILITY (CYCLO,1USAMSU) The experiment was performed at the C2215 1 16 National Superconducting Cyclotron Laboratory, MichiganC2215 1 17 State University. C2215 1 18 SAMPLE Sample was a deuterated polyethylene target (CD2)n C2215 1 19 with thickness of (10.7+-0.8)mg/cm2 C2215 1 20 DETECTOR (MAGSP) Recoil products were identified with the S800 C2215 1 21 spectrograph downstream of the GRETINA array. The C2215 1 22 S800 was run in focused mode in order to allow a C2215 1 23 large momentum acceptance. The data acquisition was C2215 1 24 triggered either by recoil-gamma coincidences between C2215 1 25 GRETINA and the first scintillator at the focal plane C2215 1 26 of the S800 spectrograph C2215 1 27 (HPGE) Gamma rays were measured using GRETINA (Gamma- C2215 1 28 Ray Energy Tracking Inbeam Nuclear Array). GRETINA C2215 1 29 detectors positioned at laboratory angles of 58 deg C2215 1 30 and 90 deg. C2215 1 31 METHOD (COINC) Coincidence of recoil products detected in C2215 1 32 S800 focal plane scintillator and gamma rays detected C2215 1 33 in GRETINA detectors was required. Inverse kinematics C2215 1 34 was used. C2215 1 35 INC-SOURCE The 30MeV/u 26Al13+ beam was produced inflight via C2215 1 36 fragmentation reactions using a primary beam of C2215 1 37 150MeV/u, 112 pnA 36Ar18+ ions to bombard a C2215 1 38 1960mg/cm2 thick Be target. The A1900 high-resolution C2215 1 39 fragment separator selected the ions of interest C2215 1 40 based on the momentum/charge, p/q, ratio after they C2215 1 41 had passed through a 600mg/cm2 thick Al wedge The C2215 1 42 26Al beam had a high purity (98+-2)% and an average C2215 1 43 intensity of (8.1+-0.4E+5 particles per second. C2215 1 44 ERR-ANALYS (DATA-ERR) No information on source of uncertainties C2215 1 45 HISTORY (20160512C) Compiled by S.H. C2215 1 46 ENDBIB 44 0 C2215 1 47 NOCOMMON 0 0 C2215 1 48 ENDSUBENT 47 0 C2215 199999 SUBENT C2215002 20160512 C160C2215 2 1 BIB 3 9 C2215 2 2 REACTION ((1-H-2(13-AL-26,N)14-SI-27,PAR,SIG)= C2215 2 3 (13-AL-26(D,N)14-SI-27,PAR,SIG)) C2215 2 4 STATUS (TABLE) Data taken from tab. 1 of the reference C2215 2 5 LEVEL-PROP (14-SI-27,E-LVL=5547.3,SPIN=4.5,PARITY=+1.) C2215 2 6 (14-SI-27,E-LVL=6734.0,SPIN=5.5,PARITY=+1.) C2215 2 7 (14-SI-27,E-LVL=7129.0,SPIN=6.5,PARITY=+1.) C2215 2 8 (14-SI-27,E-LVL=7590.1,SPIN=4.5,PARITY=+1.) C2215 2 9 (14-SI-27,E-LVL=7651.9,SPIN=5.5,PARITY=-1.) C2215 2 10 (14-SI-27,E-LVL=7739.3,SPIN=4.5,PARITY=+1./-1.) C2215 2 11 ENDBIB 9 0 C2215 2 12 COMMON 1 3 C2215 2 13 EN C2215 2 14 MEV/A C2215 2 15 30.0 C2215 2 16 ENDCOMMON 3 0 C2215 2 17 DATA 5 6 C2215 2 18 E-LVL E-LVL-ERR DATA DATA-ERR DATA-MAX C2215 2 19 KEV KEV MICRO-B MICRO-B MICRO-B C2215 2 20 5547.3 0.1 520. 110. C2215 2 21 6734.0 0.2 390. 90. C2215 2 22 7129.0 0.2 630. 130. C2215 2 23 7590.1 0.9 37. C2215 2 24 7651.9 0.6 280. 70. C2215 2 25 7739.3 0.4 70. 30. C2215 2 26 ENDDATA 8 0 C2215 2 27 ENDSUBENT 26 0 C2215 299999 ENDENTRY 2 0 C221599999999